Range radial

The phase relationship of each point of imbalance is the third factor that must be known. Balancing instruments isolate each point of imbalance and determine their phase relationship. Plotting each point of imbalance on a polar plot does this. In simple terms, a polar plot is a circular display of the shaft end. Each point of imbalance is located on the polar plot as a specific radial, ranging from 0 to 360°. 

From the above mentioned data it follows that the destructing action of microorganisms on wood impregnated with pyrolysis oils in the case of L. lepideus is almost twice as intensive as in the case of C. puteana. According to comparative plots, both cultures cause some decrease in the volume of the wider pores Fig. 2,A). However, in the case of L. lepideus, in, contrast to C puteana, a minor volume of pores in the radial range 1.5-2.1 nm appears. 

After exposure of impregnated and leached samples to C puteana and L. lepideus, the picture is being changed in the case of C puteana, they exhibit a dramatic increase in A (by 38.5%) and a (by 42%), respectively. Moreover, some increase in a is observed. A considerable alteration in the structure, i.e. a new pore volume in the radial range 1.8-2.5 nm (mesopores) appears (Fig. 2,B, 3,A). Obviously, the increase in the accessible surface of the specimen impregnated with oil after leaching facilitates the destruction process upon the contact with this microorganism. 

Fig. 6.2. Schematic drawing for the definition of depth, spread, radial range, longitudinal projected range, transverse projected range, and path length (Eckstein 1991)...

Figure 4. (a) The angular distribution of the stresses very close to the crack tip. The dots are numerical results for a material with scE/ao 3, Ho O.lno, m 0.01 and v 0.25, and the solid lines are the result for an isotropic elastic solid. Note that the 1/v r radial dependence has been accounted for within the normalization, (b) The angular distribution of remanent strains very close to the crack tip from the same computation. The numerical results plotted in both figures are for all integration stations within the radial range 8 x lO i , < r < 1.3 x 10 i ,. 

For the development of basis sets, the radial behavior of the orbitals is important, because it determines the range of exponents of the Gaussian functions that are used, and to what extent the exponent sets for different shells overlap, particularly those for electron correlation. Because the f shell is fairly compact, any basis set must cover a radial range that extends from that of the f shell to that of the outer valence s and d shells. The radial behavior is elaborated below. 

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